Particle ID was successfully reconstructed from 4 GeV data,
C1<100&&C2<100.
X-Axis : (TDCstrip3_left + TDCstrip3_right) - (TDCSci_BNL_1
+ TDCSci_BNL_2)
Y-Axis: No. of Count
Right Peak: Proton
Left Peak: Other Particles
CUTs: Cherenkov1<100&&Cherenkov2<100, for cleanup electrons.
Note: X value is related to particles' time-of-flight, proton has
heaver mass therefore distributes to far side.
Conclusion: MRPCs' timing resolution is good enough to separate Proton
from other particles, even before slewing correction. Time-of-flight
difference between the two peaks is consistent with our estimation.
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Fig 1: Proton Peak by Cherenkov C1
and C2 Selection, Module #1 |
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Fig 2: Proton Peak by Cherenkov C1
and C2 Selection, Module #2 |
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Fig 3: Proton Peak by Cherenkov C1
and C2 Selection, Module 1 && Module 2 Coincidence |
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